3,382 research outputs found

    In-Medium Effects on K0 Mesons in Relativistic Heavy-Ion Collisions

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    We present the transverse momentum spectra and rapidity distributions of π\pi^{-} and KS0^0_S in Ar+KCl reactions at a beam kinetic energy of 1.756 A GeV measured with the spectrometer HADES. The reconstructed KS0^0_S sample is characterized by good event statistics for a wide range in momentum and rapidity. We compare the experimental π\pi^{-} and KS0^0_S distributions to predictions by the IQMD model. The model calculations show that KS0^0_S at low tranverse momenta constitute a particularly well suited tool to investigate the kaon in-medium potential. Our KS0^0_S data suggest a strong repulsive in-medium K0^0 potential of about 40 MeV strength.Comment: 10 pages, 10 figures, accepted by Phys. Rev.

    An upper limit on hypertriton production in collisions of Ar(1.76 AGeV)+KCl

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    A high-statistic data sample of Ar(1.76 AGeV)+KCl events recorded with HADES is used to search for a hypertriton signal. An upper production limit per centrality-triggered event of 1.041.04 x 10310^{-3} on the 3σ3\sigma level is derived. Comparing this value with the number of successfully reconstructed Λ\Lambda hyperons allows to determine an upper limit on the ratio NΛ3H/NΛN_{_{\Lambda}^3H}/N_{\Lambda}, which is confronted with statistical and coalescence-type model calculations

    Lambda hyperon production and polarization in collisions of p(3.5 GeV) + Nb

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    Results on Λ\Lambda hyperon production are reported for collisions of p(3.5 GeV) + Nb, studied with the High Acceptance Di-Electron Spectrometer (HADES) at SIS18 at GSI Helmholtzzentrum for Heavy-Ion Research, Darmstadt. The transverse mass distributions in rapidity bins are well described by Boltzmann shapes with a maximum inverse slope parameter of about 9090\,MeV at a rapidity of y=1.0y=1.0, i.e. slightly below the center-of-mass rapidity for nucleon-nucleon collisions, ycm=1.12y_{cm}=1.12. The rapidity density decreases monotonically with increasing rapidity within a rapidity window ranging from 0.3 to 1.3. The Λ\Lambda phase-space distribution is compared with results of other experiments and with predictions of two transport approaches which are available publicly. None of the present versions of the employed models is able to fully reproduce the experimental distributions, i.e. in absolute yield and in shape. Presumably, this finding results from an insufficient modelling in the transport models of the elementary processes being relevant for Λ\Lambda production, rescattering and absorption. The present high-statistics data allow for a genuine two-dimensional investigation as a function of phase space of the self-analyzing Λ\Lambda polarization in the weak decay Λpπ\Lambda\rightarrow p \pi^-. Finite negative values of the polarization in the order of 520%5-20\,\% are observed over the entire phase space studied. The absolute value of the polarization increases almost linearly with increasing transverse momentum for pt>300p_t>300\,MeV/c and increases with decreasing rapidity for y<0.8y < 0.8.Comment: accepted by Eur. Phys. J.

    Subthreshold Xi- Production in Collisions of p(3.5 GeV)+Nb

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    Results on the production of the double-strange cascade hyperon Ξ\mathrm{\Xi^-} are reported for collisions of p\,(3.5~GeV)\,+\,Nb, studied with the High Acceptance Di-Electron Spectrometer (HADES) at SIS18 at GSI Helmholtzzentrum for Heavy-Ion Research, Darmstadt. For the first time, subthreshold Ξ\mathrm{\Xi^-} production is observed in proton-nucleus interactions. Assuming a Ξ\mathrm{\Xi^-} phase-space distribution similar to that of Λ\mathrm{\Lambda} hyperons, the production probability amounts to PΞ=(2.0±0.4(stat)±0.3(norm)±0.6(syst))×104P_{\mathrm{\Xi^-}}=(2.0\,\pm0.4\,\mathrm{(stat)}\,\pm 0.3\,\mathrm{(norm)}\,\pm 0.6\,\mathrm{(syst)})\times10^{-4} resulting in a Ξ/(Λ+Σ0)\mathrm{\Xi^-/(\Lambda+\Sigma^0)} ratio of $P_{\mathrm{\Xi^-}}/\ P_{\mathrm{\Lambda+\Sigma^0}}=(1.2\pm 0.3\,\mathrm{(stat)}\pm0.4\,\mathrm{(syst)})\times10^{-2}.Availablemodelpredictionsaresignificantlylowerthantheestimated. Available model predictions are significantly lower than the estimated \mathrm{\Xi^-}$ yield.Comment: 6 pages, 3 figure

    Intersecting Brane Worlds -- A Path to the Standard Model ?

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    In this review we describe the general geometrical framework of brane world constructions in orientifolds of type IIA string theory with D6-branes wrapping 3-cycles in a Calabi-Yau 3-fold. These branes generically intersect in points on the internal space, and the patterns of intersections govern the chiral fermion spectra. We discuss how the open string spectra in intersecting brane models are constructed, how the Standard Model can be embedded, and also how supersymmetry can be realized in this class of string vacua. After the general considerations we specialize the discussion to the case of orbifold backgrounds with intersecting D6-branes and to the quintic Calabi-Yau manifold. Then, we discuss parts of the effective action of intersecting brane world models. Specifically we compute from the Born-Infeld action of the wrapped D-branes the tree-level, D-term scalar potential, which is important for the stability of the considered backgrounds as well as for questions related to supersymmetry breaking. Second, we review the recent computation concerning of gauge coupling unification and also of one-loop gauge threshold corrections in intersecting brane world models. Finally we also discuss some aspects of proton decay in intersecting brane world models.Comment: 31 pages, To appear in the proceedings of the RTN-workshop ``The quantum structure of spacetime and the geometric nature of fundamental interactions'', September 2003 in Copenhagen, revised version contains new refs and one corrected equatio

    Baryonic resonances close to the Kbar-N threshold: the case of Sigma(1385)^+ in pp collisions

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    We present results of an exclusive measurement of the first excited state of the Sigma hyperon, Sigma(1385)^+, produced in p+p -> Sigma^+ + K^+ + n at 3.5 GeV beam energy. The extracted data allow to study in detail the invariant mass distribution of the Sigma(1385)^+. The mass distribution is well described by a relativistic Breit-Wigner function with a maximum at m_0 = 1383.2 +- 0.9 MeV/c^2 and a width of 40.2 +- 2.1 MeV/c^2. The exclusive production cross-section comes out to be 22.27 +- 0.89 +- 1.56 +3.07 -2.10 mu b. Angular distributions of the Sigma(1385)^+ in different reference frames are found to be compatible with the hypothesis that 33 % of Sigma(1385)^+ result from the decay of an intermediate Delta^{++} resonance.Comment: 12 pages; 12 figures; submitted to PR

    The Infrared Behaviour of the Pure Yang-Mills Green Functions

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    We review the infrared properties of the pure Yang-Mills correlators and discuss recent results concerning the two classes of low-momentum solutions for them reported in literature; i.e. decoupling and scaling solutions. We will mainly focuss on the Landau gauge and pay special attention to the results inferred from the analysis of the Dyson-Schwinger equations of the theory and from "{\it quenched}" lattice QCD. The results obtained from properly interplaying both approaches are strongly emphasized.Comment: Final version to be published in FBS (54 pgs., 11 figs., 4 tabs

    Strong Coupling BCS Superconductivity and Holography

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    We attempt to give a holographic description of the microscopic theory of a BCS superconductor. Exploiting the analogy with chiral symmetry breaking in QCD we use the Sakai-Sugimoto model of two D8 branes in a D4 brane background with finite baryon number. In this case there is a new tachyonic instability which is plausibly the bulk analog of the Cooper pairing instability. We analyze the Yang-Mills approximation to the non-Abelian Born-Infeld action. We give some exact solutions of the non-linear Yang-Mills equations in flat space and also give a stability analysis, showing that the instability disappears in the presence of an electric field. The holograhic picture also suggests a dependence of TcT_c on the number density which is different from the usual (weak coupling) BCS. The flat space solutions are then generalized to curved space numerically and also, in an approximate way, analytically. This configuration should then correspond to the ground state of the boundary superconducting (superfluid) ground state. We also give some preliminary results on Green functions computations in the Sakai - Sugimoto model without any chemical potentialComment: minor revisions, numerical analysis has been redone to obtain some solutions to the complete set of equations, version accepted in Nuclear Physics
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